Abstract

A novel group of interleaved orthogonal frequency division multiplexing (IL-OFDM) and partial transmission IL-OFDM (PT-IL-OFDM) schemes are proposed for optical coherent detection. In the interleaved operation, the odd (or even) subcarriers of an OFDM symbol are reserved (closed). Such an interleaved arrangement can gain the tolerance toward phase noise induced interchannel interference (PN-ICI). Meanwhile, the peak to average power ratio (PAPR) of an OFDM signal can be significantly reduced. However, half of the capacity is sacrificed for the interleaved operation. By exploring the time domain symmetry property of IL-OFDM, the concept of PT-IL-OFDM is proposed to double the capacity of IL-OFDM. Consequently, PT-IL-OFDM can gain the merits of low PAPR and a high tolerance toward PN-ICI without capacity sacrifice. Numerical simulation verified the advanced properties of IL-OFDM and PT-IL-OFDM.

© 2014 Optical Society of America

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[CrossRef]

D. Qian, N. Cvijetic, J. Hu, and T. Wang, IEEE Photon. Technol. Lett. 21, 1265 (2009).
[CrossRef]

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[CrossRef]

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[CrossRef]

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[CrossRef]

J. Lightwave Technol.

Opt. Express

Other

J. Zhao and A. D. Ellis, Optical Fiber Communication Conference, OSA Technical Digest (Optical Society of America, 2010), paper OMR1.9.

S. C. J. Lee, F. Breyer, S. Randel, D. Cardenas, H. P. A. van den Boom, and A. M. J. Koonen, in Optical Fiber Communication Conference, OSA Technical Digest (Optical Society of America, 2009), paper OWM2.

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Figures (5)

Fig. 1.
Fig. 1.

Phase noise induced intercarrier interference of traditional OFDM and interleaved OFDM.

Fig. 2.
Fig. 2.

Simulation principle of traditional OFDM (T-OFDM), interleaved OFDM (IL-OFDM), and partial transmission IL-OFDM (PT-IL-OFDM).

Fig. 3.
Fig. 3.

CCDF for T-OFDM, IL-OFDM, and PT-IL-OFDM.

Fig. 4.
Fig. 4.

EVMs of T-OFDM, IL-OFDM, and PT-IL-OFDM versus combined linewidths.

Fig. 5.
Fig. 5.

EVMs of PT-IL-OFDM ((I)FFT size=64), T-OFDM ((I)FFT size=32) versus OSNRs.

Tables (2)

Tables Icon

Table 1. Parameters of OFDM Modulationsa

Tables Icon

Table 2. Physical Parameters

Equations (4)

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Sρ(f)=α2πf2,
S(n)=1Nk=00.5*N1X2k+1ej2π(2k+1)nN,n=0,1,2,,N1.
S(n+N2)=1Nk=00.5*N1X2kej2π2k*(n+N/2)N,=1Nk=00.5*N1X2kej2π2knN+2πk,=S(n).
S(t+TIL2)=S(t),t(0,TIL2],

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